Image stitching for a multi-head printer

ABSTRACT

Techniques are disclosed for stitching images printed by a multi-head printer in a manner that is relatively insensitive to misregistration of the image segments. When a pair of overlapping print heads print a pair of adjacent image segments which meet in a stitching region, printing at each location in the stitching region is accomplished by both print heads with a weighting that depends on the location being printed within the stitching region. In one embodiment, for example, the output of each print head is weighted by a linear function of horizontal pixel position. Techniques are also disclosed for selecting screening patterns for use when stitching is performed with variable-dot printers. Such screening patterns are selected to minimize variations in density that may arise as the result of cross-web and/or down-web misregistration.

BACKGROUND

1. Field of the Invention

The present invention relates to multi-head thermal printers and, in particular, to thermal printers in which multiple print heads are used to print a single image in the form of multiple joined segments

2. Related Art

Various kinds of printers are well-known in the computing and digital image arts. Such printers include, for example dot-matrix printers, laser printers, inkjet printers and thermal printers. The focus of the present discussion is on thermal printers, so-named because they use thermal energy (heat) to produce printed output. More specifically, thermal printers typically contain a linear array of heating elements (also referred to herein as “print head elements”) that print on an output medium by, for example, transferring pigment from a donor sheet to the output medium or by initiating a color-forming reaction in the output medium. The output medium is typically a porous receiver receptive to the transferred pigment, or a paper coated with the color-forming chemistry. Each of the print head elements, when activated, forms color on the medium passing underneath the print head element, creating a spot having a particular density. Regions with larger or denser spots are perceived as darker than regions with smaller or less dense spots. Digital images are rendered as two-dimensional arrays of very small and closely-spaced spots.

A thermal print head element is activated by providing it with energy. Providing energy to the print head element increases the temperature of the print head element, causing either the transfer of pigment to the output medium or the formation of color in the receiver. The density of the output produced by the print head element in this manner is a function of the amount of energy provided to the print head element. The amount of energy provided to the print head element may be varied by, for example, varying the amount of power to the print head element within a particular time interval or by providing power to the print head element for a longer time interval.

A single thermal printer may include multiple thermal print heads, which may, for example, be staggered with respect to each other. One example of this kind of printer is described in U.S. Pat. No. 4,660,052 to Kaiya et al., and is described as a heat sensitive recording apparatus with multiple thermal heads disposed in a staggered arrangement along two platen rollers. The apparatus has alternate image segments printed on a first platen roller by a first set of print heads. The intervening segments are filled in by a second set of print heads printing on a second platen roller. The heads are arranged such that the printing of the second set of print heads overlaps the printing of the first set of print heads, forming “stitching” regions between each pair of adjacent segments in which the printing may be adjusted to obscure the presence of a transition from one to the other. In this patent, the method of joinery is described as a simple abutment in which a point of transition is chosen near the center of each stitching region. All pixels to the left of the transition are printed by the left-hand print head of the pair of overlapping heads, and all, pixels to the right of the transition points are printed by the right-hand print head of the pair. This method of joinery is troublesome, because it lacks robustness toward imperfections in the printer hardware. For example, if the paper motion is not perfectly perpendicular to the print heads, then the paper may shift slightly to the right or left when traveling from one set of print heads to the other, thereby opening a gap in the stitch or causing an overlap of image segments. In addition to these mechanical imperfections, the thermal print head heats up as it prints, and thermal expansion of the heads can cause a visible overlap of image segments.

U.S. Pat. No. 4,997,410 to Onuki and Denda describes specific means for implementing an abutted joint as described above by means that distribute stitching-region data to the appropriate print heads, depending on whether they are to the right or left of a chosen transition point. This patent describes means for manual readjustment of the stitch so as to eliminate any visible gap or overlap, and also describes means for automatically compensating for the effects of thermal expansion of the heads. It would be preferable that no such manual adjustments were required for proper operation.

U.S. Pat. No. 5,119,108 to Hatakeyama describes a very similar system, but adds the recommendation that the image segments be overlapped by 2-4 pixels, thereby eliminating (for all practical purposes) the possibility of a gap opening up between the image segments. This, of course introduces a 2-4 pixel wide region of higher printed density, which the inventors apparently consider to to be unobjectionable due to the very narrow width of the overlap. This imperfection, however, extends the full length of the image, and may be visible despite its narrow width.

A solution to this problem is proposed in U.S. Pat. No. 5,450,099 to Stephenson and Fiscella. This patent describes a stitch that is more sophisticated than the simple abutted joint. On each line in the stitching region, the pixels to be printed are divided in a random pattern between the two print heads. Each print head prints approximately one-half of the pixels in the stitch, interleaved so that each pixel is printed either by one or by the other of the two print heads. On each line, the random division of pixels is changed so that there is no recurring pattern from line to line. This avoids correlated defects that extend the full length of the image, but it does place demands on the mechanical and thermal tolerances of the printer, as a misregistration of the patterns will result in significant uncontrolled changes in the printed density of the stitch region. In the case of misregistration, approximately 25% of the pixels will be printed by both print heads, and 25% of the pixels will not be printed by either print head. These randomly occurring increases and decreases of density do not compensate for each other, and an imperfect density is printed.

In view of the drawbacks of these prior-art methods of stitching image segments in thermal printers, there is a need for a method of joining image segments such that mechanical imperfections in the printer hardware, and thermal expansion of the printer components, will not result in visible artifacts in the printed image. The consequence of such a method would be an improvement of image quality, and a reduction in the cost of wide-format thermal printers (since a high-precision transport mechanism would not be required).

SUMMARY

Techniques are disclosed for stitching images printed by a multi-head printer in a manner that is relatively insensitive to misregistration of the image segments. When a pair of overlapping print heads print a pair of adjacent image segments which meet in a stitching region, printing at each location in the stitching region is accomplished by both print heads with a weighting that depends on the location being printed within the stitching region. In one embodiment, for example, the output of each print head is weighted by a linear function of horizontal pixel position. Techniques are also disclosed for selecting screening patterns for use when stitching is performed with variable-dot printers. Such screening patterns are selected to minimize variations in density that may arise as the result of cross-web and/or down-web misregistration.

Other features and advantages of various aspects and embodiments of the present invention will, become apparent from the following description and from the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A is a diagrammatic representation of an image region in which two sub-regions are printed by a multi-head printer using a prior-art abutment joint and in which the two sub-regions meet exactly at the center of a stitching-region;

FIG. 1B is a diagrammatic representation of an image region in which two sub-regions are printed by a multi-head printer using a prior-art abutment joint and in which a horizontal misregistration has caused the two sub-regions to partially overlap within the stitching region;

FIG. 2 is a graph illustrating the relationship between pixel position and density in the image region illustrated in FIG. 1A;

FIG. 3 is a graph illustrating the relationship between pixel position and density in the image region illustrated in FIG. 1B;

FIG. 4 is a graph illustrating weighting functions that are applied to overlapping print heads according to one embodiment of the present invention and the resulting total output density when no misregistration occurs;

FIG. 5 is a graph illustrating weighting functions that are applied to overlapping print heads according to one embodiment of the present invention and the resulting total output density when a horizontal misregistration occurs;

FIGS. 6A-6F are graphs illustrating the application of embodiments of the present invention to non-uniform image data;

FIGS. 7A-7B illustrate dot patterns arranged in rectangular grids;

FIG. 7C illustrates the dot patterns of FIGS. 7A-7B overlapped in a dot-on-dot arrangement;

FIG. 7D illustrates the dot patterns of FIGS. 7A-7B overlapped in a dot-off-dot arrangement;

FIG. 8A illustrates a dot pattern in a staggered arrangement;

FIG. 8B illustrates a dot pattern in a rectangular arrangement

FIG. 8C illustrates the dot patterns of FIGS. 8A-8B overlapping with each other;

FIG. 9A illustrates four example pixels, each of which includes a single dot in a distinct one of four dot positions;

FIG. 9B illustrates a pattern formed from a repeating pattern of the four pixels shown in FIG. 9A;

FIGS. 9C-9E illustrate three four-pixel patterns that may be used to perform screening according to embodiments of the present invention;

FIG. 10 illustrates a superimposition of two different four-pixel patterns;

FIG. 11 illustrates a superimposition of two different three-pixel, patterns with a vertical misregistration; and

FIGS. 12A-12D illustrate four different five-pixel patterns that may be used to perform screening according to various embodiments of the present invention.

DETAILED DESCRIPTION

Techniques are disclosed for stitching images printed by a multi-head printer in a manner that is relatively insensitive to misregistration of the image segments. When a pair of overlapping print heads print a pair of adjacent image segments which meet in a stitching region, printing at each location in the stitching region is accomplished by both print heads with a weighting that depends on the location being printed within the stitching region. In one embodiment, for example, the output of each print head is weighted by a linear function of horizontal pixel position. Techniques are also disclosed for selecting screening patterns for use when stitching is performed with variable-dot printers. Such screening patterns are selected to minimize variations in density that may arise as the result of cross-web and/or down-web misregistration.

In various embodiments of the present invention, techniques are provided for use in a printer to stitch images in a manner that is relatively insensitive to small and unintended misregistration of the image segments. The misregistration may be either “down-web” (i.e., in the direction of the paper motion), or “cross-web” (i.e., transverse to the paper motion, and along the print heads).

Referring to FIG. 1A, an image region 100 is shown in diagrammatic form for purposes of example. The region 100 represents a region of an image printed by a multi-head printer using a simple abutment joint, as described above. Region 100 includes two sub-regions 102 a-b. In the present example, region 102 a is printed by a first print head 106 a and region 102 b is printed by a second print head 106 h in a thermal printer. Print heads 106 a-h are illustrated in block form for ease of illustration. Paper moves through the printer in the direction indicated by arrow 108. The patterns illustrated within regions 102 a-b are provided merely for purposes of example. In actual implementation, the regions 102 a-b may include any image data.

Region 100 also includes a sub-region 104 in which print heads 106 a and 106 b overlap. The overlapping region 104 is also referred to herein as a “stitching region.” or, more simply, as a “stitch.” For ease of illustration and explanation, the contents of the regions 102 a-b are illustrated in FIG. 1 using hatch patterns to represent image data having constant and equal densities. FIG. 1A illustrates the case in which the region 100 is printed with perfect registration, and in which the image segments printed by heads 106 a-b therefore meet exactly at the center line 110 of the stitching region 104 without overlapping. In the case of perfect registration, therefore, center line 110 indicates the point at which one print head stops printing and the other one begins.

According to various embodiments of the present inventions, images may be stitched in a manner that is relatively insensitive to small and unintended misregistration of the image segments (e.g., the regions 102 a-b) by abandoning the requirement that each pixel in the stitching region 104 be printed by either one of the print, heads 106 a-b or by the other. Instead, printing at each location in the stitching region 104 is accomplished by both print heads 106 a-b, and with a weighting that depends on the location within the stitching region 104. On the left-hand side of the stitching region 104, the media is printed primarily by the left-hand print head 106 a, and on the right-hand side of the stitching region 104 it is printed primarily by the right-hand print head 106 b. In this fashion, there is a gradual transition across the stitching region 104 from one of the print heads 106 a-b to the other.

A schematic illustration of the difference between the traditional abutted joint, and the “graded” joint disclosed herein is made in FIGS. 2-3. It is assumed in FIGS. 2-3 that one is attempting to print a constant density across the stitching region 104. Referring to FIG. 2, for example, a graph 200 is shown which illustrates the relationship between pixel position and density in the case of an abutted joint, in which an abrupt transition is made from one of the print heads 106 a-b to the other at the center of the stitching region 104 (as shown in FIG. 1A). Curve 204 a illustrates the density printed by the first print head 106 a, curve 204 b illustrates the density printed by the second print head 106 b, and curve 206 illustrates the combined density of curves 204 a and 204 b.

In the case of an abutted joint, each of the two overlapping print heads 106 a-b prints up to the transition point (at the center of stitching region 104 in FIG. 1A), but not beyond. When the paper is moving perfectly from one platen to the other, and the temperature is well controlled, then one may adjust the positions of the print heads 106 a-b, and the transition point on each print head, so that the transition is perfect, resulting in a net density that is perfectly uniform across the stitching region 104. This case is illustrated in FIG. 1A and by curve 206 in FIG. 2, which is uniform for all positions.

If, however, the print, heads 106 a-b expand, or if the paper path is imperfect, the printing from the second print head 106 b may unintentionally overlap the printing of the first print head 106 a, yielding an overlap region of higher density. Referring to FIG. 1B, for example, an image region 120 is shown which is similar to the image region 100 of FIG. 1A. For example, the region 120 includes sub-regions 122 a-b printed by print heads 106 a-b, respectively, on an output medium moving in direction 108. The region 120 also includes a stitching region 124. For purposes of the present discussion, the contents of the stitching region 124 are illustrated in FIG. 1B to indicate that the patterns shown in regions 122 a and 122 b are printed at the same densities within stitching region 124 as those printed outside of the stitching region 124.

As shown in FIG. 1B, sub-regions 122 a-b overlap within a sub-region 112 of stitching region 124 as a result of horizontal misregistration. As indicated in FIG. 1B, as a result of this misregistration, the right edge 110 a of the sub-region 122 a (printed by print head 106 a) is to the right of the left edge 110 b of the sub-region 122 b (printed by print head 106 b), causing the sub-regions 122 a-b to overlap in the region 112. This overlap causes the overlap region 112 to be of higher density than either region 122 a or 122 b.

Referring to FIG. 3, a graph 300 is shown which illustrates the relationship between pixel position and density in the case the region 120 shown in FIG. 1B. Curve 304 a illustrates the density printed by the first print head 126 a, curve 304 b illustrates the density printed by the second print head 126 b, and curve 306 illustrates the combined density of curves 304 a and 304 h. As illustrated by curve 306, the overlap between the output printed by the two print heads 126 a-b causes the total density to spike within the overlap region 112, which is a sub-region of the stitching region 124. Alternatively, the paper or print mechanism may move or distort in such a way that a gap develops between the regions 122 a-b, leading to a narrow region of very low density (not shown).

In the following discussion of various embodiments of the present invention, reference will be made to output produced by the print heads 106 a-b. Although the print heads 106 a-b are illustrated in FIGS. 1A-1B as producing output using prior art techniques, the same print heads 106 a-b may be controlled to produce output according to various embodiments of the present invention. Furthermore, to the extent that the techniques disclosed herein may require modification to the print heads 106 a-b, any description of such techniques should he interpreted to refer to appropriately-modified print heads rather than to the prior art print heads 106 a-b.

Referring to FIG. 4, a graph 400 is shown which illustrates the relationship between pixel position and density in the case of images printed according to various embodiments of the present invention. Curve 404 a illustrates the density printed by the first print head 106 a, curve 404 b illustrates the density printed by the second print head 106 b, and 406 illustrates the combined density of curves 404 a and 404 b.

In FIG. 4, the dashed lines indicate a corresponding stitching region 403 in the output image. To the left of the stitching region 408 the left-hand print head 106 a prints the desired density, and within the stitching region 408 the left-hand print head 106 a prints a density that is graded from full, density to zero density. By the same token, the right-hand print head 106 b prints the desired density to the right of the stitching region 408, and within the stitching region 408 the right-hand print head 106 b prints a lower density, graded from right to left in such a way that the combination of the density printed by the left and right print heads 106 a-b combines to form the desired density. Although in FIG. 4 the curves 404 a-b are linear and have equal and opposite slopes within the stitching region 408, this is not a limitation of the present invention. Rather, as will be described in more detail below, other weighting functions may be used to combined the output of the print heads 106 a-b within the stitching region 408.

When the paper path is perfect, as in the example shown in FIG. 4, and the temperature is well controlled, the printing method just described results in a density that is uniform across the stitching region 408, just as in the case of the abutted joint. However, in the case of a misregistration, the density change that results from the printing method described above with respect to FIG. 4 extends over many pixels and is of much lower amplitude than in the case of a misregistration when an abutted joint is used.

For example, referring to FIG. 5, a graph 500 is shown which illustrates the relationship between pixel position and density in the case of images printed according to various embodiments of the present invention when there is a misregistration. The meaning of curves 504 a-b and 506 are the same as curves 404 a-b and 406 (FIG. 4), respectively.

Assuming for example that the stitching region 508 is 100 pixels wide, a misregistration of 1 pixel results in a density change of only about 1%, peaking in the center of the stitching region 508. In the case that the image segments move apart from each other, no gap appears between them. Instead, there is a small decrease of density in the misregistered region (again about 1% for a 1 pixel misregistration).

This method applies even when the printed material itself is not uniform across the stitching region. In the more general case, the image data in each line will vary across the stitch, as illustrated in FIGS. 6A-6F. Referring to FIG. 6A, for example, a graph 600 is shown in which a curve 604 represents image data to be printed. As shown in FIG. 6A, curve 604 varies in density across stitching region 608.

Referring to FIG. 6B, a graph 610 is shown in which a curve 614 represents a linear weighting function to be applied to the output of the first print head 106 a. Similarly, referring to FIG. 6C, a graph 620 is shown in which a curve 624 represents a linear weighting function to be applied to the output of the second print head 106 b. The curves 614 and 624 show that fraction of the density that will be printed by the print heads 106 a-b, respectively.

Referring to FIGS. 6D-6E, graphs 630 and 640 illustrate the result of multiplying the image data 604 by the weight functions 614 and 624, respectively, and represent the densities to be printed by the print heads 106 a-b, respectively. Referring to FIG. 6F, graph 650 combines graphs 600 (FIG. 6A), 630 (FIG. 6D), and 640 (FIG. 6E), and thereby illustrates how the desired total image density 604 is composed from the densities printed by each of the print heads 106 a-b (illustrated by graphs 634 and 644, respectively).

In order to implement this method of stitching, it is necessary to consider the details of the printing 700 method being used. Generally speaking, there are two classes of thermal printing methods, referred to as “variable-density” and “variable-dot” printing. In variable-density printing, each pixel is filled with a uniform dye density; this uniform density changes as heat is applied to the medium. In variable-dot printing, a dot of maximum density is formed in the pixel; the size of the dot increases as heat is applied. The apparent printed density in a variable-dot printer is determined primarily by the fraction of the printed surface covered by ink. In actuality, printers are not ideal, and may print pixels that are neither uniformly filled with dye nor perfect dots of maximum density. However, so-called “dye diffusion thermal transfer” (D2T2) printers are generally considered to be variable-density in nature, and wax-transfer thermal printers are best described as variable-dot.

The techniques described above may be applied in a straightforward way to variable-density printers, although the densities printed by the two print heads 106 a-b may not he perfectly additive. Those of ordinary skill in the art will appreciate that in the event of imperfect additivity of the two print heads 106 a-b, the resulting printed density may be lower or higher than the intended density, and that modification of the weighting functions for the two print heads 106 a-b may be used to compensate for the imperfection.

For variable-dot printers, however, there is a further complication arising from the printing of isolated dots. In particular, in variable-dot printers the printed density in the stitch depends sensitively on whether the dots printed by one print head fall on top of, or in between, the dots printed by another print bead. The former case is referred to as “dot-on-dot” printing, and the latter as “dot-off-dot” printing.

For example, referring to FIGS. 7A-7B, to image segments 702 a-b are shown, each of which is printed in a rectangular grid. Although the dots in the image segments 702 a-b are shown as having different sizes and patterns, this is merely to make the two sets of dots distinguishable from each other. The dots in image segments 702 a-b are intended to represent dots having the same size and density. The dot sizes shown represent mid-tone densities, for which density shifts from misregistration are most significant. Dots of larger size may overlap both when registered and when misregistered, and may even extend into adjacent pixels. In these cases, the term “dot-off-dot” may be taken to mean the registration giving minimum overlap. Significant overlaps of this type tend to subdue density variations and are not illustrated here. Referring to FIG. 70, an image 702 c representing a simple dot-on-dot overlap of the images 702 a-b is shown.

A shift of the image segments 702 a-b by one-half pixel with respect to each other will change the merged image 702 c from a complete dot-on-dot overlap to a nearly dot-off-dot overlap. This situation is shown by image segment 702 d in FIG. 7D. Likewise, a down-web misalignment of dots can also move the dots from complete dot-on-dot alignment to nearly dot-off-dot alignment.

The density change resulting from this change in registration may be large. If we take the fill-factor of the dots printed by each of the print heads 106 a-b to be “f”, the density inside the dot to be “Dmax”, and the density outside the dot to be “Dmin”, then the apparent printed density on each side of the stitch is shown by Equation 1.

D=−log₁₀

(1−f)·10^(−D) ^(min) +f·10^(−D) ^(max)

  Equation 1

it should be appreciated that Equation 1 is approximate and should be taken only as an estimate of the magnitude of the density changes that will occur. Equation 1 does not, for example, consider scattering or multiple reflections in the medium.

For the purposes of estimation, we may take Dmin to be 0, and Dmax to be about 2, so that this result becomes as shown in Equation 2.

D=−log₁₀

(1−f)+f·10^(−D) ^(max)

≈−log₁₀(1−f)  Equation 2

provided that f is not close to 1. This means that the apparent density depends primarily on the fill factor. In a dot-on-dot situation the fill factor in the stitch region is approximately the same for the overlapped segments as for the individual unweighted image segments. On the other hand, when the two segments are dot-off-dot (and provided that the dots are not large enough to overlap in the dot-off-dot situation) then the fill factor is doubled. In particular, the situation for small values of f is indicated by Equation 3:

D≈−log₁₀(e)log_(e)(1−f)≈f·log₁₀(e)  Equation 3

This effect means that the production of a desired density in the stitch as a combination of the weighted density of two overlapping segments is quite difficult for a variable-dot printer, because it requires a knowledge of whether the printing is dot-on-dot or dot-off-dot (or somewhere between). This, in turn, requires precision control of the paper transport and of thermal expansion, thereby potentially counteracting the benefits of the techniques described above.

A very small change in the printed patterns can change this situation significantly. For example, referring to FIGS. 8A-8B, two image segments 802 a-b are shown. The second image segment 802 b (FIG. 88) (like the image segment 702 b shown in FIG. 78) is printed in a rectangular grid. The first image segment 802 a (FIG. 8A), however, is printed with its dots staggered. Referring to FIG. 80, an image 802 c representing an overlap of the images 802 a-b is shown.

Staggering the positions of the dark black dots in image 802 a creates a situation in which only half of the dots in the overlap region of the image 802 c are dot-on-dot. Although it is still true that a cross-web shift of a half-pixel will take us to a nearly dot-off-dot situation, in the image 802 c there is no positioning that leads to a completely dot-on-dot configuration. In other words, the change in fill factor from dot-on-dot to dot-off-dot has been reduced by about 2, compared to the situation illustrated in FIGS. 7A-7D. It also true that down-web misregistration in the situation illustrated in FIGS. 8A-8C leads to smaller variations, since a shift of a half-pixel in that direction brings us from 50% dot-on-dot overlap back to another 50% dot-on-dot overlap, and there is no position (for dots of the size illustrated) in that direction for which the printing is entirely dot-off-dot.

This effect can be further improved by identifying improved dot patterns. In principle, the dot placement may be varied in both the cross-web and the down-web direction, but conventional print heads have uniform pixel spacing, and the design of the printer is simplified if all the print heads have the same pixel spacing. Therefore, the discussion is limited to the case in which the dot position is only varied in the down-web direction, although this is not a limitation of the present invention.

In this case, it is always possible to achieve complete dot-off-dot printing for small dots by shifting the image segments cross-web so that their columns interlace. Departures from this alignment will lead to various degrees of dot-on-dot printing. The best patterns are those that limit the maximum amount of dot-on-dot overlap, since this will limit, the density variation between the full dot-off-dot printing alignment and maximum dot-on-dot alignment.

There is also a second constraint, not satisfied by the example described above with respect to FIGS. 8A-8C. Namely, when the screening described herein is being used to stitch two image segments, it is desirable that the two segments have patterns that are similar enough that the response curves and thermal corrections will be the same for all image segments. In the example just given with respect to FIGS. 8A-8C, a rectangular pattern (FIG. 8B) was combined with a staggered pattern (FIG. 8A) These two patterns are typically different in both response curve and thermal corrections, and this makes the control of printed density and color from one of the segments 802 a-b to the next quite complicated. Fortunately, in many cases there are distinct patterns with symmetries that make them equivalent in these aspects.

For ease of explanation, the following discussion is restricted to dot patterns in which dot location within a pixel is chosen from among a set of N equally spaced down-web locations or “phases,” and the sequence of locations is a repeating pattern in the lateral direction. This is not, however, a limitation of the present invention.

Consider, for example, the case in which N=4. In this case there are four equally spaced down-web locations for the dot within the pixel. Referring to FIG. 9A, four example pixels 902 a-d are shown, each of which includes a single dot in a distinct one of the four dot positions (phases). Phases are illustrated in FIG. 9A, and in the remaining figures, using dashed lines on which dots are centered. The particular dot shapes and sizes used in the drawings are shown merely for purposes of example. More generally, dots may be of any shape and grow outward to any size.

The phases may be numbered from 1 to 4, for example, and may be used in any repeating order. In this illustration, the length of the repeating order will be limited to the number of phases, so that each phase will be represented exactly once in the sequence. The sequences may then be labeled by the sequence of phases. For example, the label 1 3 2 4 refers to the repeating sequence of phases “1 3 2 4 1 3 2 4 1 3 2 4 . . . ” and will result in lines of pixels forming a pattern 910 shown in FIG. 95. The entire pattern 910 is signified by just four numbers giving the order of the four phases, in this case 1 3 2 4.

Since there are 4!=24 different ways of arranging four numbers, one might conclude that there are 24 different patterns available for the 4-phase system. However, there are actually only three different patterns, because many of the 24 patterns are equivalent. For example, if the pattern above (1 3 2 4) had been described starting in the second column rather than the first, it would have been called 3 2 4 1, although this clearly describes the same pattern. In other words, any cyclic permutation of the four numbers in a pattern leads to an equivalent pattern.

By the same token, if one describes the same pattern but starting at different phase positions, the result is another set of labels that is different from but equivalent to the original set of labels. For example, moving one phase position up-web turns the label 1 3 2 4 into 2 4 3 1, as may be seen visually from observing FIG. 95. This is the result of adding 1 to each number in the original label, and taking the results modulo 4.

Following these two rules for finding equivalent labels, we find that the 16 labels shown in Table 1 all describe exactly the same pattern:

TABLE 1 Cross-Web Shifts Down-Web Shifts 1 3 2 4 3 2 4 1 2 4 1 3 4 1 3 2 2 4 3 1 4 3 1 2 3 1 2 4 1 2 4 3 3 1 4 2 1 4 2 3 4 2 3 1 2 3 1 4 4 2 1 3 2 1 3 4 1 3 4 2 3 4 2 1

In other words, of 24 possible labels, 16 are equivalent and describe a single physical pattern. The remaining 8 fall into two groups of 4, and then represent diagonal lines of positive and negative slope, as follows:

Pattern 1: 1 2 3 4→2 3 4 1→3 4 1 2→4 1 2 3

Pattern 2: 4 3 2 1→3 2 1 4→2 1 4 3→1 4 3 2

These two groups have only 4 members rather than 16 because the down-web shifts, in these cases, leads to the same labels as the cross-web shifts.

Therefore, in conclusion, the N=4 case has lust three distinct patterns. Referring to FIGS. 9C-9E, examples 920 a-c of each such pattern are shown. Any one of these three patterns 920 a-c may be used on one of the print heads in a stitch, and another on the other print head. However, the performance will not be equivalent for all pairs. It is desirable to find two patterns with the property that, no matter what the misregistration, the maximum amount of dot-on-dot overlap is as small as possible. It is, of course, true that no matter which two patterns are chosen, there is always some registration in which at least one dot of one pattern is directly on top of one dot of the other (one dot per repeat unit, that is). Therefore, we know that the best we achieve is that, independent of registration, no more than one dot per repeat unit of the first pattern ever falls directly on top of a dot in the repeat unit of the other.

Consider, for example, the second and third patterns 920 b-c in the case N=4. These two patterns have the property that although they are distinct, they have a vertical symmetry that, ensures that they will share a common response curve and thermal control characteristics. However, it is not true that they overlap by only one pixel per unit cell independent of registration. The superposition of the two patterns 920 b-c can lead to situations in which two of the four dots per unit cell are registered. Referring to FIG. 10, an example of such a superimposition 1000 of the two patterns 920 b-e is shown.

The same turns out to be true of any two of the N=4 Patterns. This leads, then, to the question whether there are any values of N for which there are patterns that overlap by at most one pixel per repeat unit. This is a question that may be resolved, for example, by computer modeling. Those of ordinary skill in the art, for example, will understand how to implement a software program to generate all possible patterns for a particular value of N and to determine which, if any, of such patterns have a worst-case overlap of one dot per repeat unit. If any such patterns are found, such patterns may be searched to determine whether they include any pairs of patterns which are related by a symmetry which signals that they are thermally equivalent (i.e., will have the same gamma curve and thermal history control). Table 2 lists results obtained for several values of N using such a computer modeling approach.

TABLE 2 Number of Number Number of pattern pairs of Number of Distinct with single dot Phases N Permutations Patterns overlap 3 6 2 1 4 24 3 0 5 120 8 6 6 720 24 0 7 5040 108 27

Examples will now be described of pattern pairs which satisfy the criteria just described when the number N of phases is odd. For example, the case of N=3 phases has two patterns, containing the exemplar labels 1 2 3 and 3 2 1. When these two patterns are plotted, they appear as shown in the image segment 1100 in FIG. 11. The image segment 1100 represents a randomly selected registration.

When these two patterns are misregistered horizontally or vertically, there is no relative position at which more than one dot per unit-cell (the unit-cell being three dots in size) is coincident. This is a benefit to both cross-web and down-web misregistration, as it limits the range of density variations that may occur.

In the case of N=5 there are eight distinct patterns. Four of these patterns have the mutual property of not overlapping by more than one dot per unit-cycle. Referring to FIGS. 12A-12D, examples 1200 a-d of each of the patterns are shown. From the symmetry of these patterns 1200 a-d, we discern that the first and second patterns 1200 a-b will share the same response curve and thermal characteristics. The same is true of the third and fourth patterns 1200 c-d.

It should be evident that the use of phase patterns to modify the location of printed dots on the line will introduce a small amount of distortion into the printed image. Those of ordinary skill in the art will recognize that this distortion may be removed by resampling the image before printing to arrive at estimates for the image data at the phase-shifted pixel positions at which printing will actually occur.

It is to be understood that although the invention has been described above in terms of particular embodiments, the foregoing embodiments are provided as illustrative only, and do not limit or define the scope of the invention. Various other embodiments, including but not limited to the following, are also within the scope of the claims.

Although the dots in the examples above are circular, this is not a limitation of the present invention. Other dot shapes that may be used include, for example, elliptical dots which are wider than they are tall. When such dots are used there will be less interstitial horizontal space for dots to move into if horizontal misregistration occurs.

Although the examples provided above are described in relation to density screening, the same techniques may be applied to color screening in color images. In this case, each color may be independently stitched according to the techniques just described. The overlaid printing of these color separations then leads to a full color image. It is important to note, however, that each of the color planes is in its entirety a variable-dot image, and that its registration with respect to other color planes will affect the color of the printed images. Therefore, it is valuable to use the screening of image segments not only to improve the quality of the stitches, but also to reduce the variability of image density and color. Since there is generally no issue of balancing the thermal properties of different color planes, this may be done by using stitches with different numbers of phases on the different color planes, or by using the same number of phases but different pairs of patterns on each plane. The result will be color planes with reduced seam visibility, and with reduced color shift with misregistration.

Although the examples above involve repeating patterns of uniformly-sized phases, the present invention is not limited to use in conjunction with such patterns. Rather, embodiments of the present invention may, for example, be used with non-repeating patterns and/or with patterns having phases of non-uniform size.

The techniques described above may be implemented, for example, in hardware, software, firmware, or any combination thereof. The techniques described above may be implemented in one or more computer programs executing on a programmable computer including a processor, a storage medium readable by the processor (including, for example, volatile and non-volatile memory and/or storage elements), at least one input device, and at least one output device. Program code may be applied to input, entered using the input device to perform the functions described and to generate output. The output may be provided to one or more output devices.

Each computer program within the scope of the claims below may be implemented in any programming language, such as assembly language, machine language, a high-level procedural programming language, or an object-oriented programming language. The programming language may, for example, be a compiled or interpreted programming language.

Each such computer program may be implemented in a computer program product tangibly embodied in a machine-readable storage device for execution by a computer processor. Method steps of the invention may be performed by a computer processor executing a program tangibly embodied on a computer-readable medium to perform functions of the invention by operating on input and generating output. Suitable processors include, by way of example, both general and special purpose microprocessors. Generally, the processor receives instructions and data from a read-only memory and/or a random access memory. Storage devices suitable for tangibly embodying computer program instructions include, for example, all forms of non-volatile memory, such as semiconductor memory devices, including EPROM, EEPROM, and flash memory devices; magnetic disks such as internal hard disks and removable disks; magneto-optical disks; and CD-ROMs. Any of the foregoing may be supplemented by, or incorporated in, specially-designed ASICs (application-specific integrated circuits) or Field-Programmable Gate Arrays (FPGAs). A computer can generally also receive programs and data from a storage medium such as an internal disk or a removable disk. These elements will also be found in a conventional desktop or workstation computer as well as other computers suitable for executing computer programs implementing the methods described herein, which may be used in conjunction with any digital print engine or marking engine, display monitor, or other raster output device capable of producing color or gray scale pixels on paper, film, display screen, or other output medium. 

1. A method for screening a region in a digital image, the method comprising steps of; (A) dividing the region into a two-dimensional array of cells having n columns and m rows, wherein m≧2; (B) for each column in the array, selecting a first corresponding phase shift; and (C) for each cell in the array, performing steps of: (1) identifying the column containing the cell; (2) identifying the first corresponding phase shift selected for the identified column; and (3) printing a dot centered at a location in the cell corresponding to the identified first corresponding phase shift. 2-56. (canceled) 